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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2013 Jun 15;69(Pt 7):m385–m386. doi: 10.1107/S1600536813015651

Bis(dicyanamido-κN)[tris­(3-amino­propyl)amine-κ4 N]nickel(II)

Jun Luo a, Xin-Rong Zhang a, Li-Juan Qiu a, Feng Yang a, Bao-Shu Liu a,*
PMCID: PMC3772421  PMID: 24046564

Abstract

In the title complex, [Ni(C2N3)2(C9H24N4)], the NiII atom is coordinated in a distorted octa­hedral geometry by one tris­(3-amino­prop­yl)amine (tris­apa) ligand and two dicyanamide (dca) ligands [one of them disordered in a 0.681 (19):0319 (19) ratio]. Inter­molecular N—H⋯N hydrogen bonds involving the N atoms of the dca anions and the tris­apa amine H atoms result in the formation of a three-dimensional network.

Related literature  

For magnetic properties and structural types of dicyanamide complexes, see: Batten (2005); Batten & Murray (2003); Batten et al. (1998); Ghosh et al. (2011); Ion et al. (2013); Manson et al. (1999); Mastropietro et al. (2013); Turner et al. (2011). For dicyanamide complexes with multidentate Schiff bases, see: Sadhukhan et al. (2011); Fondo et al. (2011); Bhar et al. (2011). For dicyanamide complexes with polyamines as co-ligands, see: Khan et al. (2011). For Ni—N bond lengths in aliphatic amine nickel complexes, see: Cho et al. (2002); Brezina et al. (1999) and in [Ni(tn)2{C2N3}](ClO4)(tn is tri­methyl­enedi­amine, see: Li et al. (2002). graphic file with name e-69-0m385-scheme1.jpg

Experimental  

Crystal data  

  • [Ni(C2N3)2(C9H24N4)]

  • M r = 379.13

  • Monoclinic, Inline graphic

  • a = 10.171 (1) Å

  • b = 11.3960 (11) Å

  • c = 15.5305 (15) Å

  • β = 105.660 (2)°

  • V = 1733.3 (3) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 1.14 mm−1

  • T = 213 K

  • 0.17 × 0.09 × 0.05 mm

Data collection  

  • Bruker SMART APEX CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2000) T min = 0.830, T max = 0.945

  • 12722 measured reflections

  • 4056 independent reflections

  • 3403 reflections with I > 2σ(I)

  • R int = 0.024

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.027

  • wR(F 2) = 0.079

  • S = 1.07

  • 4056 reflections

  • 269 parameters

  • 20 restraints

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 0.38 e Å−3

  • Δρmin = −0.32 e Å−3

Data collection: SMART (Bruker, 2000); cell refinement: SAINT (Bruker, 2000); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL.

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536813015651/bg2508sup1.cif

e-69-0m385-sup1.cif (20.3KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813015651/bg2508Isup2.hkl

e-69-0m385-Isup2.hkl (198.8KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
N2—H2C⋯N10i 0.92 (2) 2.38 (2) 3.255 (2) 160 (2)
N2—H2D⋯N10ii 0.80 (2) 2.43 (2) 3.193 (2) 158 (2)
N3—H3D⋯N10i 0.90 (2) 2.36 (2) 3.154 (2) 148 (2)
N4—H4D⋯N7iii 0.90 (3) 2.19 (3) 3.094 (3) 176 (2)

Symmetry codes: (i) Inline graphic; (ii) Inline graphic; (iii) Inline graphic.

Acknowledgments

This project was supported by the National Natural Science Foundation of China. (NSFC 20571086).

supplementary crystallographic information

Comment

Recently, dicyanamide complexes have attracted considerable interest because of their fascinating magnetic properties and diverse structural types (Turner et al., 2011; Batten et al., 2005; Batten et al., 2003). For example, the binary transition metal dicyanamide complexes display long-range magnetic ordering, with the nature of the ordering dependent on the particular metal ion involved. Thus the Cr (47 K) and Mn (16 K) compounds are antiferromagnets (Manson et al., 1999), while the Co (9 K) and Ni systems (21 K) are ferromagents (Batten et al., 1998). It is well known that the structure and the magnetic property of the complexes are related to the nature of the co-ligands (Ghosh et al., 2011; Mastropietro et al., 2013; Ion et al., 2013). Although a great effort is focused on studies of dicyanamide complexes with multidentate schiff bases (Sadhukhan et al., 2011; Fondo et al., 2011; Bhar et al., 2011), few dicyanamide complexes with polyamines as co-ligands have been reported recently (Khan et al., 2011). To further study the effect of the nature of co-ligands on the structures and properties of dicyanamide complexes, we herein report the synthesis and crystal structure of the title new nickel dicyanamide complex [Ni(trisapa)(C2N3)2] (I).

The nickel ion in I is coordinated by four N atoms from the tris(3-aminopropyl) amine and two terminal N atoms from two dicyanamide anions to form a distorted octahedral geometry, in which the equatorial plane is formed by the three N atoms(N2, N3, N4) of tris(3-aminopropyl)amine and one nitrile N atom (N8) of a monodentate (disordered) dicyanamide, where the disorder atoms are C12 and C12', N9 and N9', C13 and C13' respectively. The two apical sites are occupied by one trisapa N atom(N1) and one nitrile N atom (N5) of another monodentate dicyanamide (Fig. 1). Table. 2 shows the intermolecular hydrogen interactions between the uncoordinated N atoms of dicyanamide anions and the amine H atoms of trisapa, responsible of the construction of a three-dimensional network (Fig. 2). The Ni—N (trisapa) distances (2.100 (2)–2.196 (1) Å) are rather different, with values similar to the corresponding distances in the aliphatic amine nickel complexes (Cho et al., 2002; Brezina et al., 1999). The apical Ni—N (dicyanamide) distance(2.145 (1) Å) is slightly longer than the basal Ni—N(dicyanamide) distance(2.090 (2) Å). These distances in I are comparable to the corresponding ones in [Ni(tn)2{C2N3}](ClO4)(tn is trimethylenediamine, Li et al., 2002). In I, N—Ni—N cis angles range from 89.36 (7)° to 90.37 (6)° (basal-basal) and 84.32 (6)° to 95.61 (6)° (basal-apical), indicating that the distortion from an ideal octahedral geometry in I is not serious.

Experimental

A 4 ml ethanol solution of tris(3-aminopropyl)amine(0.10 mmol, 18.83 mg) and a 4 ml e thanol solution of nickel nitrate(0.10 mmol, 29.08 mg) were mixed and stirred for 5 min, the mixed solution was pale-blue. To the mixture was added a 2 ml aqueous solution of sodium dicyanamide (0.20 mmol, 17.81 mg). After stirred for another 5 min, the solution was filtered and the filtrate was slowly evaporated in air. After one week, blue block crystals of I were isolated in 34% yield. Anal: Calculated for C13H24N10Ni: C 41.18%, H 6.38%, N 36.95%. Found C 40.86%, H 6.47%, N 37.07%.

Refinement

One of the dicyanamide units is disordered in two halves, which were refined with restraints (both metric as in displacement factors). The corresponding occupation factors refined to 0.681/0.319 (19). The amine H atom were found from difference maps and refined freely with a final N—H range 0.80 (2) Å - 0.92 (2) Å. Remaining H atoms were placed in geometrically idealized positions and constrained to ride on their parent atoms with C—H distances of 0.98 Å and Uiso(H) = 1.2 × U(Host) .

Figures

Fig. 1.

Fig. 1.

View of the molecule of I showing the atom-labelling scheme. Displacement ellipsoids are drawn at the 50% probability level. In open bonds, the minor disordered part of the molecule. H atoms not shown, for clarity.

Fig. 2.

Fig. 2.

Three dimensional network in I formed by hydrogen-bonding interactions.

Crystal data

[Ni(C2N3)2(C9H24N4)] F(000) = 800
Mr = 379.13 Dx = 1.453 Mg m3
Monoclinic, P21/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 5066 reflections
a = 10.171 (1) Å θ = 2.3–27.7°
b = 11.3960 (11) Å µ = 1.14 mm1
c = 15.5305 (15) Å T = 213 K
β = 105.660 (2)° Block, blue
V = 1733.3 (3) Å3 0.17 × 0.09 × 0.05 mm
Z = 4

Data collection

Bruker SMART APEX CCD area-detector diffractometer 4056 independent reflections
Radiation source: fine-focus sealed tube 3403 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.024
φ and ω scans θmax = 27.8°, θmin = 2.1°
Absorption correction: multi-scan (SADABS; Bruker, 2000) h = −11→13
Tmin = 0.830, Tmax = 0.945 k = −14→14
12722 measured reflections l = −20→19

Refinement

Refinement on F2 Primary atom site location: structure-invariant direct methods
Least-squares matrix: full Secondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.027 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.079 H atoms treated by a mixture of independent and constrained refinement
S = 1.07 w = 1/[σ2(Fo2) + (0.0475P)2 + 0.0784P] where P = (Fo2 + 2Fc2)/3
4056 reflections (Δ/σ)max = 0.006
269 parameters Δρmax = 0.38 e Å3
20 restraints Δρmin = −0.32 e Å3

Special details

Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.
Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)

x y z Uiso*/Ueq Occ. (<1)
Ni1 0.75943 (2) 0.944842 (17) 0.199688 (12) 0.01927 (8)
N1 0.78081 (14) 0.76691 (11) 0.25612 (9) 0.0232 (3)
N2 0.63129 (16) 0.88585 (14) 0.07694 (9) 0.0274 (3)
H2C 0.541 (2) 0.8859 (18) 0.0774 (13) 0.034 (5)*
H2D 0.636 (2) 0.9404 (16) 0.0450 (14) 0.024 (5)*
N3 0.58711 (15) 0.98960 (13) 0.24394 (10) 0.0230 (3)
H3C 0.605 (2) 1.0556 (15) 0.2735 (13) 0.020 (5)*
H3D 0.525 (2) 1.0082 (19) 0.1927 (15) 0.035 (5)*
N4 0.88525 (17) 1.02601 (14) 0.31382 (11) 0.0296 (3)
H4C 0.921 (2) 1.0799 (19) 0.2941 (15) 0.038 (6)*
H4D 0.829 (2) 1.0540 (17) 0.3450 (16) 0.038 (6)*
N5 0.73577 (17) 1.11767 (13) 0.14290 (10) 0.0325 (3)
N6 0.6910 (2) 1.31289 (14) 0.07638 (12) 0.0460 (4)
N7 0.7027 (2) 1.38147 (16) −0.07076 (12) 0.0514 (5)
N8 0.93047 (16) 0.91772 (14) 0.15190 (11) 0.0336 (3)
N10 1.32388 (17) 0.95680 (15) 0.08290 (11) 0.0370 (4)
C1 0.7900 (2) 0.67980 (16) 0.18584 (13) 0.0344 (4)
H1A 0.8050 0.6020 0.2137 0.041*
H1B 0.8709 0.6988 0.1656 0.041*
C2 0.6680 (2) 0.67200 (16) 0.10390 (13) 0.0373 (4)
H2A 0.6733 0.5982 0.0726 0.045*
H2B 0.5842 0.6700 0.1235 0.045*
C3 0.6591 (2) 0.77285 (18) 0.03917 (12) 0.0372 (4)
H3A 0.7453 0.7786 0.0227 0.045*
H3B 0.5864 0.7567 −0.0154 0.045*
C4 0.67169 (19) 0.72696 (15) 0.29801 (12) 0.0304 (4)
H4A 0.7062 0.7383 0.3628 0.037*
H4B 0.6595 0.6423 0.2876 0.037*
C5 0.53150 (19) 0.78395 (14) 0.26810 (12) 0.0285 (4)
H5A 0.5000 0.7812 0.2027 0.034*
H5B 0.4674 0.7378 0.2914 0.034*
C6 0.5276 (2) 0.90978 (15) 0.29799 (13) 0.0318 (4)
H6A 0.4328 0.9326 0.2925 0.038*
H6B 0.5786 0.9166 0.3611 0.038*
C7 0.91496 (19) 0.75441 (16) 0.32628 (13) 0.0336 (4)
H7A 0.9885 0.7577 0.2965 0.040*
H7B 0.9179 0.6764 0.3533 0.040*
C8 0.9448 (2) 0.84521 (17) 0.40100 (12) 0.0374 (4)
H8A 0.8609 0.8602 0.4188 0.045*
H8B 1.0125 0.8130 0.4530 0.045*
C9 0.9974 (2) 0.96002 (16) 0.37472 (13) 0.0350 (4)
H9A 1.0369 1.0069 0.4284 0.042*
H9B 1.0693 0.9446 0.3450 0.042*
C10 0.71677 (18) 1.20685 (15) 0.10710 (11) 0.0271 (4)
C11 0.6993 (2) 1.34348 (16) −0.00333 (13) 0.0342 (4)
N9 1.0877 (5) 0.8948 (10) 0.0568 (4) 0.066 (2) 0.681 (19)
C12 1.0075 (9) 0.9122 (9) 0.1113 (6) 0.0352 (18) 0.681 (19)
C13 1.2146 (8) 0.9299 (11) 0.0737 (6) 0.0328 (15) 0.681 (19)
N9' 1.1203 (14) 0.8524 (7) 0.1020 (17) 0.063 (4) 0.319 (19)
C12' 1.027 (2) 0.8940 (19) 0.1275 (14) 0.048 (6) 0.319 (19)
C13' 1.2234 (14) 0.915 (2) 0.0963 (13) 0.031 (3) 0.319 (19)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Ni1 0.01766 (12) 0.02156 (12) 0.01955 (12) −0.00006 (8) 0.00666 (8) 0.00235 (7)
N1 0.0205 (7) 0.0213 (6) 0.0279 (7) 0.0009 (5) 0.0069 (5) 0.0020 (5)
N2 0.0251 (8) 0.0366 (8) 0.0214 (7) −0.0007 (6) 0.0077 (6) 0.0019 (6)
N3 0.0240 (7) 0.0213 (7) 0.0256 (7) 0.0011 (6) 0.0100 (6) 0.0000 (6)
N4 0.0286 (8) 0.0293 (8) 0.0288 (8) −0.0061 (7) 0.0039 (6) 0.0000 (6)
N5 0.0375 (9) 0.0319 (8) 0.0303 (8) 0.0003 (7) 0.0131 (7) 0.0089 (6)
N6 0.0673 (13) 0.0314 (8) 0.0454 (10) 0.0115 (8) 0.0256 (9) 0.0137 (7)
N7 0.0540 (12) 0.0509 (11) 0.0462 (10) −0.0011 (9) 0.0080 (9) 0.0253 (9)
N8 0.0250 (8) 0.0422 (8) 0.0369 (8) −0.0008 (7) 0.0139 (7) 0.0003 (7)
N10 0.0255 (9) 0.0523 (10) 0.0350 (9) −0.0021 (7) 0.0113 (7) −0.0009 (7)
C1 0.0341 (10) 0.0251 (9) 0.0456 (11) 0.0076 (7) 0.0135 (8) −0.0032 (7)
C2 0.0378 (11) 0.0320 (9) 0.0435 (10) −0.0030 (8) 0.0134 (8) −0.0172 (8)
C3 0.0337 (10) 0.0519 (11) 0.0271 (9) −0.0036 (9) 0.0103 (8) −0.0150 (8)
C4 0.0333 (10) 0.0267 (8) 0.0323 (9) −0.0058 (7) 0.0106 (7) 0.0050 (7)
C5 0.0291 (9) 0.0268 (8) 0.0337 (9) −0.0078 (7) 0.0156 (7) −0.0030 (7)
C6 0.0398 (11) 0.0269 (8) 0.0366 (10) −0.0033 (8) 0.0241 (8) −0.0021 (7)
C7 0.0253 (9) 0.0320 (9) 0.0397 (10) 0.0043 (7) 0.0022 (8) 0.0099 (8)
C8 0.0323 (10) 0.0454 (11) 0.0281 (9) −0.0045 (8) −0.0029 (7) 0.0113 (8)
C9 0.0279 (10) 0.0427 (11) 0.0292 (9) −0.0070 (8) −0.0013 (7) 0.0043 (7)
C10 0.0255 (9) 0.0330 (9) 0.0248 (8) −0.0011 (7) 0.0104 (7) 0.0034 (7)
C11 0.0291 (10) 0.0302 (9) 0.0405 (10) 0.0000 (7) 0.0046 (8) 0.0097 (8)
N9 0.039 (2) 0.117 (5) 0.051 (3) −0.030 (2) 0.029 (2) −0.044 (3)
C12 0.023 (3) 0.045 (5) 0.040 (2) −0.003 (2) 0.013 (2) −0.012 (2)
C13 0.031 (2) 0.050 (4) 0.021 (3) −0.0063 (18) 0.0128 (17) −0.008 (3)
N9' 0.055 (5) 0.040 (4) 0.117 (10) −0.004 (3) 0.062 (6) −0.018 (4)
C12' 0.021 (6) 0.018 (4) 0.107 (14) −0.006 (4) 0.021 (8) −0.005 (6)
C13' 0.034 (5) 0.044 (6) 0.025 (8) 0.003 (4) 0.025 (5) −0.005 (6)

Geometric parameters (Å, º)

Ni1—N8 2.090 (2) C1—H1A 0.9800
Ni1—N4 2.100 (2) C1—H1B 0.9800
Ni1—N2 2.108 (1) C2—C3 1.513 (3)
Ni1—N3 2.111 (1) C2—H2A 0.9800
Ni1—N5 2.145 (1) C2—H2B 0.9800
Ni1—N1 2.196 (1) C3—H3A 0.9800
N1—C1 1.497 (2) C3—H3B 0.9800
N1—C4 1.501 (2) C4—C5 1.521 (3)
N1—C7 1.506 (2) C4—H4A 0.9800
N2—C3 1.474 (2) C4—H4B 0.9800
N2—H2C 0.92 (2) C5—C6 1.511 (2)
N2—H2D 0.80 (2) C5—H5A 0.9800
N3—C6 1.474 (2) C5—H5B 0.9800
N3—H3C 0.87 (2) C6—H6A 0.9800
N3—H3D 0.90 (2) C6—H6B 0.9800
N4—C9 1.476 (2) C7—C8 1.523 (3)
N4—H4C 0.82 (2) C7—H7A 0.9800
N4—H4D 0.90 (3) C7—H7B 0.9800
N5—C10 1.150 (2) C8—C9 1.511 (3)
N6—C10 1.300 (2) C8—H8A 0.9800
N6—C11 1.311 (3) C8—H8B 0.9800
N7—C11 1.142 (3) C9—H9A 0.9800
N8—C12 1.132 (6) C9—H9B 0.9800
N8—C12' 1.18 (1) N9—C13 1.309 (8)
N10—C13 1.124 (7) N9—C12 1.339 (7)
N10—C13' 1.20 (1) N9'—C12' 1.22 (2)
C1—C2 1.522 (3) N9'—C13' 1.29 (2)
N8—Ni1—N4 89.36 (7) C1—C2—H2B 108.8
N8—Ni1—N2 90.14 (6) H2A—C2—H2B 107.7
N4—Ni1—N2 172.26 (6) N2—C3—C2 112.5 (1)
N8—Ni1—N3 174.36 (6) N2—C3—H3A 109.1
N4—Ni1—N3 89.38 (7) C2—C3—H3A 109.1
N2—Ni1—N3 90.37 (6) N2—C3—H3B 109.1
N8—Ni1—N5 90.09 (6) C2—C3—H3B 109.1
N4—Ni1—N5 85.28 (6) H3A—C3—H3B 107.8
N2—Ni1—N5 87.00 (6) N1—C4—C5 118.7 (1)
N3—Ni1—N5 84.32 (6) N1—C4—H4A 107.6
N8—Ni1—N1 90.16 (6) C5—C4—H4A 107.6
N4—Ni1—N1 95.61 (6) N1—C4—H4B 107.6
N2—Ni1—N1 92.11 (6) C5—C4—H4B 107.6
N3—Ni1—N1 95.43 (5) H4A—C4—H4B 107.1
N5—Ni1—N1 179.08 (6) C6—C5—C4 114.3 (2)
C1—N1—C4 108.3 (1) C6—C5—H5A 108.7
C1—N1—C7 104.0 (1) C4—C5—H5A 108.7
C4—N1—C7 106.8 (1) C6—C5—H5B 108.7
C1—N1—Ni1 109.9 (1) C4—C5—H5B 108.7
C4—N1—Ni1 116.6 (1) H5A—C5—H5B 107.6
C7—N1—Ni1 110.4 (1) N3—C6—C5 111.2 (1)
C3—N2—Ni1 120.0 (1) N3—C6—H6A 109.4
C3—N2—H2C 108 (1) C5—C6—H6A 109.4
Ni1—N2—H2C 112 (1) N3—C6—H6B 109.4
C3—N2—H2D 112 (1) C5—C6—H6B 109.4
Ni1—N2—H2D 101 (1) H6A—C6—H6B 108.0
H2C—N2—H2D 103 (2) N1—C7—C8 116.3 (2)
C6—N3—Ni1 122.8 (1) N1—C7—H7A 108.2
C6—N3—H3C 107 (1) C8—C7—H7A 108.2
Ni1—N3—H3C 108 (1) N1—C7—H7B 108.2
C6—N3—H3D 111 (1) C8—C7—H7B 108.2
Ni1—N3—H3D 102 (1) H7A—C7—H7B 107.4
H3C—N3—H3D 105 (2) C9—C8—C7 113.3 (2)
C9—N4—Ni1 120.4 (1) C9—C8—H8A 108.9
C9—N4—H4C 106 (2) C7—C8—H8A 108.9
Ni1—N4—H4C 104 (2) C9—C8—H8B 108.9
C9—N4—H4D 109 (1) C7—C8—H8B 108.9
Ni1—N4—H4D 106 (1) H8A—C8—H8B 107.7
H4C—N4—H4D 111 (2) N4—C9—C8 110.2 (2)
C10—N5—Ni1 175.1 (2) N4—C9—H9A 109.6
C10—N6—C11 122.4 (2) C8—C9—H9A 109.6
C12—N8—Ni1 166.7 (6) N4—C9—H9B 109.6
C12'—N8—Ni1 175 (1) C8—C9—H9B 109.6
N1—C1—C2 116.8 (2) H9A—C9—H9B 108.1
N1—C1—H1A 108.1 N5—C10—N6 172.1 (2)
C2—C1—H1A 108.1 N7—C11—N6 172.9 (2)
N1—C1—H1B 108.1 C13—N9—C12 124.3 (7)
C2—C1—H1B 108.1 N8—C12—N9 172.3 (9)
H1A—C1—H1B 107.3 N10—C13—N9 175 (1)
C3—C2—C1 113.6 (2) C12'—N9'—C13' 122 (2)
C3—C2—H2A 108.8 N8—C12'—N9' 170 (2)
C1—C2—H2A 108.8 N10—C13'—N9' 169 (2)
C3—C2—H2B 108.8

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
N2—H2C···N10i 0.92 (2) 2.38 (2) 3.255 (2) 160 (2)
N2—H2D···N10ii 0.80 (2) 2.43 (2) 3.193 (2) 158 (2)
N3—H3D···N10i 0.90 (2) 2.36 (2) 3.154 (2) 148 (2)
N4—H4D···N7iii 0.90 (3) 2.19 (3) 3.094 (3) 176 (2)

Symmetry codes: (i) x−1, y, z; (ii) −x+2, −y+2, −z; (iii) x, −y+5/2, z+1/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: BG2508).

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Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536813015651/bg2508sup1.cif

e-69-0m385-sup1.cif (20.3KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813015651/bg2508Isup2.hkl

e-69-0m385-Isup2.hkl (198.8KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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